The comparison of various electronic-optical vision systems has been c
onducted based on the criterion ultimate information capacity, C, limi
ted by fluctuations of the flux of quanta. The information capacity of
daylight, night, and thermal vision systems is determined first of al
l by the number of picture elements, M, in the optical system. Each el
ement, under a sufficient level of irradiation, can transfer about one
byte of information for the standard frame time and so C approximate
to M bytes per frame. The value of the proportionality factor, one byt
e per picture element, is referred to systems of daylight and thermal
vision, in which a photocharge in a unit cell of the imager is limited
by storage capacity, and in general it varies within a small interval
of 0.5 byte per frame for night vision systems to 2 bytes per frame f
or ideal thermal imagers. The ultimate specific information capacity,
C, of electronic vision systems under low irradiation levels rises wi
th increasing density of optical channels until the number of the irra
diance gradations that can be distinguished becomes less than two in e
ach channel. In this case, the maximum value of C turns out to be pro
portional to the flux of quanta coming from an object under observatio
n. Under a high level of irradiation, C is limited by diffraction eff
ects and amounts to l/lambda(2) bytes/cm(2) frame.